The present invention relates to an alkali-free glass substrate, having a strain point of 680° C. or higher, a Young's modulus of 78 GPa or greater, an uv transmittance at a wavelength of 300 nm of from 40% to 85% in terms of 0.5 mm thickness, an in-plane distribution of the uv transmittance at a wavelength of 300 nm in a G6-sized substrate of 1% or less in terms of 0.5 mm thickness, an average cooling rate around the glass transition point obtained according to a rate cooling method of 400° C./min or lower, and an in-plane distribution of the average cooling rate of 40° C./min or less.
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1. An alkali-free glass substrate, having a strain point of 680° C. or higher, a Young's modulus of 78 GPa or greater, an uv transmittance at a wavelength of 300 nm of from 40% to 85% in terms of 0.5 mm thickness,
wherein, at an average cooling rate around a glass transition point obtained according to a rate cooling method of 400° C./min or lower, the alkali-free glass substrate has an in-plane distribution of the uv transmittance at a wavelength of 300 nm in a substrate size of 1850 mm×1500 mm of 1% or less in terms of 0.5 mm thickness, and an in-plane distribution of the average cooling rate in the substrate size of 1850 mm×1500 mm of 40° C./min or less,
the alkali-free glass substrate comprising, on a mass percentage basis in terms of oxides:
e####
wherein MgO+CaO+SrO+BaO is from 8 to 29.5.
2. The alkali-free glass substrate according to
wherein MgO+CaO+SrO+BaO is from 13 to 22.
3. The alkali-free glass substrate according to
4. The alkali-free glass substrate according to
5. The alkali-free glass substrate according to
6. The alkali-free glass substrate according to
7. The alkali-free glass substrate according to
8. The alkali-free glass substrate according to
9. The alkali-free glass substrate according to
10. The alkali-free glass substrate according to
11. The alkali-free glass substrate according to
12. The alkali-free glass substrate according to
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This application is a continuation of U.S. application Ser. No. 14/919,814, filed on Oct. 22, 2015, which is a Continuation Application of PCT Application No. PCT/JP2014/061168, filed Apr. 21, 2014, the entire contents of which are incorporated herein by reference, which claims foreign priority to Japanese Application No. 2013-090141, filed on Apr. 23, 2013, the entire contents of which are incorporated herein by reference.
The present invention relates to an alkali-free glass substrate which is suitable as substrate glass for various kinds of displays, does not substantially contain an alkali metal oxide, and is easily formed to have a plate shape, and whose in-plane distribution of UV transmittance is suppressed.
Conventionally, substrate glass for various kinds of displays, particularly, glass on which surface a metal or oxide thin film is formed needs to be alkali-free glass which does not substantially contain alkali metal ions since film characteristics are degraded due to alkali metal ions being diffused in the thin film if an alkali metal oxide is contained.
When a flat panel display (FPD) represented by a liquid crystal display device (LCD) is produced, two sheets of substrate glass (in a case of an LCD, substrate glass provided with a TFT element and substrate glass provided with a color filter) constituting the FPD are bonded to each other by using a curable resin.
Here, since the FPD contains constituent elements such as a TFT element, which has a problem of heat resistance, a photo-curable resin is used as the curable resin and the resin is cured by applying UV rays. Accordingly, it is necessary for substrate glass for display to have UV-transmitting properties. Patent Documents 1 and 2 suggest alkali-free glass substrates whose UV transmittance at a wavelength of 300 nm is in the range of 50% to 85% in terms of 0.5 mm thickness.
The substrate glass for display preferably has a uniform UV transmittance over the entire surface of the substrate glass for display, that is, has a small in-plane distribution of UV transmittance, in addition to the UV transmittance falling within a desired range. For example, there has been a technique of polymer stabilized alignment (hereinafter, referred to as “PSA”) in which a photopolymerizable monomer is added to liquid crystal materials filling a liquid crystal layer of an LCD and is made to form a polymer in the vicinity of an alignment film by applying light in a state in which liquid crystal molecules are tilted in a predetermined direction, thereby stabilizing the molecular alignment of the liquid crystal materials (see Patent Document 3). In order to deal with this technique, it is necessary for substrate glass for display to have a small in-plane distribution of UV transmittance. In the substrate glass for display, when the in-plane distribution of UV transmittance is large, the application conditions of UV rays need to be changed depending on the region of the substrate glass for display and thus the yield of a liquid crystal display panel is decreased.
Further, in the field of an LCD or an organic EL display device (OLED), particularly, mobile display devices such as a mobile and a mobile phone, an important issue is to reduce a weight and thickness of display devices. In order to deal with this issue, it is desirable to make the plate thickness of the substrate glass for display used for a display device smaller. As a method for making the plate thickness smaller, usually applied is a method of performing an etching treatment on substrate glass by using hydrofluoric acid or the like after or before a member for a display device is formed on the surface of the substrate glass, and further thinning by a physically polishing, if necessary.
However, when the substrate glass is made thinner by performing an etching treatment or the like before a member for a display device is formed on the surface of the substrate glass, the strength of the substrate glass is degraded and the deflection amount thereof becomes larger. This causes a problem of incapability of performing a treatment in the existing production line.
In addition, when the substrate glass is made thinner by performing an etching treatment or the like after a member for a display device is formed on the surface of the substrate glass, a problem that small scratches formed on the surface of the substrate glass during the process of forming the member for a display device on the surface of the substrate glass become apparent, that is, a problem of generation of an edge pit arises.
Then, for the purpose of solving such problems, there has been proposed a method of bonding substrate glass having a small plate thickness (thin substrate glass) to another supporting substrate glass to form a laminate, performing a predetermined treatment for producing a display device in this state, and then separating the thin substrate glass from the supporting substrate glass (see Patent Document 4).
As the method of separating the thin substrate glass from the supporting substrate glass, as in the method described in Patent Document 5, a method of scan-irradiating the surface of a substrate with laser beams can be used.
In order to deal with this technique, it is necessary for the substrate glass for display to have a small in-plane distribution of light transmittance. In the substrate glass for display, when the in-plane distribution of light transmittance is large, the application conditions of laser beams need to be changed depending on the region of the substrate glass for display and thus the yield of a display device is decreased.
[Patent Document 1] JP-A-2006-36625
[Patent Document 2] JP-A-2006-36626
[Patent Document 3] JP-A-2009-53544
[Patent Document 4] JP-A-2009-184172
[Patent Document 5] JP-A-2012-104093
In recent years, for small high-resolution displays, for example, mobile terminals such as a smartphone, a method using laser annealing is employed as a method of producing high quality p-Si TFT. Further, in order to reduce the compaction, glass having a high strain point is demanded. In addition, with the tendency of increase in plate size and reduction in thickness of a glass substrate, in order to suppress the deflection of the glass substrate at the time of transportation, glass having a high Young's modulus and a high specific elastic modulus (Young's modulus/density) is demanded. An object of the present invention is to solve the above-described problems and to provide an alkali-free glass substrate having a high UV transmittance, a small in-plane distribution of the UV transmittance, a high strain point, and a high Young's modulus, and which can be easily formed to have a plate shape at the time of producing the substrate.
In order to solve the above-mentioned problem, the present invention provides an alkali-free glass substrate, having a strain point of 680° C. or higher, a Young's modulus of 78 GPa or greater, an UV transmittance at a wavelength of 300 nm of from 40% to 85% in terms of 0.5 mm thickness, an in-plane distribution of the UV transmittance at a wavelength of 300 nm in a G6-sized substrate of 1% or less in terms of 0.5 mm thickness, an average cooling rate around the glass transition point obtained according to a rate cooling method of 400° C./min or lower, and an in-plane distribution of the average cooling rate of 40° C./min or less, and containing, on a mass percentage basis in terms of oxides:
SiO2
50 to 73;
Al2O3
10.5 to 24;
B2O3
0 to 5;
MgO
0 to 10;
CaO
0 to 14.5;
SrO
0 to 24;
BaO
0 to 20;
ZrO2
0 to 5;
SnO2
0.01 to 1; and
Fe2O3
0.005 to 0.1,
in which MgO+CaO+SrO+BaO is from 8 to 29.5.
The alkali-free glass substrate of the present invention preferably has a total amount of a halogen element of from 0.001% to 1%, on a mass percentage basis in terms of oxides.
The alkali-free glass substrate of the present invention preferably has an in-plane distribution of a content of Fe (on a mass percentage basis in terms of Fe2O3) of from 0.001% to 0.003%.
In order to solve the above-mentioned problem, the present invention also provides a method of producing an alkali-free glass substrate having a SiO2—Al2O3—RO (RO is one or more kinds of MgO, CaO, BaO, and SrO)-based composition, containing:
a process of preparing glass raw materials so as to make alkali-free glass having a strain point of 680° C. or higher, a Young's modulus of 78 GPa or greater and an UV transmittance at a wavelength of 300 nm of from 40% to 85% in terms of 0.5 mm thickness, and containing, on a mass percentage basis in terms of oxides,
SiO2
50 to 73,
Al2O3
10.5 to 24,
B2O3
0 to 5,
MgO
0 to 10,
CaO
0 to 14.5,
SrO
0 to 24,
BaO
0 to 20,
ZrO2
0 to 5,
SnO2
0.01 to 1, and
Fe2O3
0.005 to 0.1,
in which MgO+CaO+SrO+BaO is from 8 to 29.5; and
a process of managing temperature conditions at the time of forming and annealing such that an average cooling rate around the glass transition point obtained according to a rate cooling method is 400° C./min or lower, an in-plane distribution of the average cooling rate is 40° C./min or less, and an in-plane distribution of the UV transmittance at a wavelength of 300 nm in a G6-sized substrate is 1% or less in terms of 0.5 mm thickness.
In the method of producing an alkali-free glass substrate of the present invention, a total amount of a halogen element is preferably from 0.001% to 1% on a mass percentage basis in terms of oxides.
In the method of producing an alkali-free glass substrate of the present invention, an in-plane distribution of a content of Fe is preferably from 0.001% to 0.003% on a mass percentage basis in terms of Fe2O3.
The alkali-free glass substrate of the present invention is easily formed to have a plate shape at the time of producing the substrate. Further, since the alkali-free glass substrate of the present invention has a high UV transmittance and a small in-plane distribution of the UV transmittance, the yield thereof is improved when used as substrate glass for FPD.
The alkali-free glass substrate of the present invention will be described.
The alkali-free glass substrate of the present invention (hereinafter, also referred to as a “glass substrate of the present invention”) contains SiO2, Al2O3, SnO2, and Fe2O3 as indispensable components and contains B2O3, MgO, CaO, SrO, BaO, and ZrO2 as optional components.
Next, the composition ranges of respective components will be described. When SiO2 is less than 50% (% by mass, the same applies hereinafter unless otherwise noted), strain point is not sufficiently increased, thermal expansion coefficient is increased, and density is increased. It is preferably 52% or greater, more preferably 54% or greater, and still more preferably 56% or greater. When it exceeds 73%, meltability at the time of producing glass is degraded, temperature T2 or temperature T4 at which glass viscosity becomes 102 dPa·s or 104 dPa·s, respectively, are increased, and devitrification temperature is increased. It is preferably 70% or less, more preferably 68.5% or less, and still more preferably 67% or less.
Al2O3 suppresses phase separation of glass, decreases thermal expansion coefficient, and increases strain point. However, when it is less than 10.5%, these effects are less likely to be exhibited, and further, since another component increasing expansion coefficient is increased, the thermal expansion of glass becomes effectively increased. It is preferably 12.5% or greater, more preferably 14.5% or greater, and still more preferably 16.5% or greater. When it exceeds 24%, meltability of glass at the time of production may become degraded or devitrification temperature may be increased. It is preferably 23% or less, more preferably 22.5% or less, and still more preferably 22% or less.
B2O3 is not indispensable, but can be contained because it improves melting reactivity of glass at the time of production, decreases devitrification temperature, and improves BHF resistance. However, when the content thereof is excessively large, strain point is decreased and Young's modulus is decreased. Accordingly, it is set to 5% or less and preferably 4% or less. In order to obtain the above-described effects, it is preferably 0.5% or greater, more preferably 0.8% or greater, still more preferably 1% or greater, and particularly preferably 1.2% or greater.
Among alkaline earths, MgO has a characteristic of increasing Young's modulus while maintaining density to be low without increasing expansion coefficient and improves meltability at the time of producing glass. Thus it can be contained. However, when the content thereof is excessively large, devitrification temperature is increased. Accordingly, it is set to 10% or less, preferably 8% or less, more preferably 7.5% or less, and still more preferably 7% or less. In order to obtain the above-described effects, it is preferably 1% or greater, more preferably 2% or greater, and still more preferably 3% or greater.
Among alkaline earths, next to MgO, CaO has a characteristic of increasing Young's modulus while maintaining density to be low without increasing expansion coefficient and improves meltability at the time of producing glass. Thus it can be contained. However, when the content thereof is excessively large, devitrification temperature may be increased or a large amount of phosphorus which is an impurity in limestone (CaCO3) serving as a raw material of CaO may be mixed. Accordingly, it is set to 14.5% or less, preferably 10% or less, more preferably 8.5% or less, and still more preferably 7% or less. In order to obtain the above-described effects, it is preferably 1% or greater, more preferably 2% or greater, and still more preferably 3% or greater.
SrO can be contained because it improves meltability at the time of producing glass without increasing devitrification temperature of the glass. However, when the content thereof is excessively large, expansion coefficient may be increased. Accordingly, it is set to 24% or less, preferably 12% or less, more preferably 10.5% or less, and still more preferably 9% or less. In order to obtain the above-described effects, it is preferably 1.5% or greater, more preferably 2% or greater, and still more preferably 2.5% or greater.
BaO is not indispensable, but can be contained in order to improve meltability at the time of producing glass. However, when the content thereof is excessively large, expansion coefficient and density of the glass are extremely increased. Accordingly, it is set to 20% or less, preferably 13.5% or less, more preferably 10% or less, still more preferably 8% or less, and particularly preferably 6% or less. In order to obtain the above-described effects, it is preferably 0.1% or greater, more preferably 0.5% or greater, and still more preferably 1% or greater.
ZrO2 is set to 5% or less in order to decrease melting temperature at the time of producing glass or to accelerate crystal deposition at the time of firing. When it exceeds 5%, the glass becomes unstable or relative dielectric constant ∈ of the glass is increased. It is preferably 1.5% or less, more preferably 1% or less, still more preferably 0.5% or less, and particularly preferably substantially not contained.
When the total content of MgO, CaO, SrO, and BaO is less than 8%, temperature T4 at which glass viscosity becomes 104 dPa·s is increased and lifetime of equipment used for forming glass in a plate shape or a housing structure of a float bath or a heater in a case of float forming may be extremely shortened. It is preferably 10% or greater, more preferably 11.5% or greater, and still more preferably 13% or greater. When it exceeds 29.5%, a problem in that thermal expansion coefficient cannot be decreased may arise. Accordingly, it is preferably 22% or less, more preferably 20% or less, and still more preferably 18% or less.
SnO2 is preferably contained in order to improve clarity at the time of producing glass. SnO2 generates O2 gas in a glass melt obtained by melting glass raw materials. In the glass melt, SnO2 is reduced to SnO at a temperature of 1450° C. or higher, generates O2 gas, and has a function of making bubbles be greatly grown. The glass raw material is preferably melted at a temperature of 1500° C. or higher for the purpose of more effectively growing bubbles. The content of Sn in the glass is 0.01% or greater in terms of SnO2. When SnO2 is less than 0.01%, the clarity effect at the time of melting glass cannot be obtained. It is preferably 0.05% or greater and more preferably 0.1% or greater. When SnO2 exceeds 1%, the glass may be colored or devitrification may occur. Therefore, the content of Sn in the glass is 1% or less, preferably 0.5% or less, and more preferably 0.3% or less, in terms of SnO2.
The content of Sn is not an amount to be added in the glass raw materials but an amount remaining in the glass melt. The same applies to the content of Fe, content of F, and content of Cl described below.
In a case where glass contains Sn4+, UV transmittance of the glass is increased due to Sn in the glass being oxidized and Fe being reduced during the process of cooling the glass.
Fe2O3 has functions of increasing temperature of molten glass in a melting tank at the time of producing glass and decreasing bed temperature in the melting tank due to infrared absorption effect of Fe2+ ions. Accordingly, the content of Fe in glass is 0.005% or greater, preferably 0.01% or greater, more preferably 0.02% or greater, and particularly preferably 0.04% or greater, in terms of Fe2O3.
When the content thereof is excessively large, this may lead to a problem of coloration of glass or decrease in UV transmittance. Accordingly, it is set to 0.1%, and preferably 0.07% or less, more preferably 0.055% or less, and particularly preferably 0.045% or less.
In the alkali-free glass substrate of the present invention, halogen elements are not dispensable, but can be contained to improve clarity at the time of producing glass. As the halogen elements to be used for this purpose, F and Cl are preferable from a viewpoint of clarity.
When the content of F is less than 0.001% by mass, the clarifying function at the time of melting glass raw materials may be decreased. Accordingly, it is preferably 0.005% by mass or greater, more preferably 0.01% by mass or greater, still more preferably 0.02% by mass or greater, and particularly preferably 0.03% by mass or greater.
When the content of F exceeds 0.15% by mass, strain point of the glass to be produced is decreased. Accordingly, it is preferably 0.12% by mass or less and more preferably 0.1% by mass or less.
When the content of Cl is less than 0.001% by mass, the clarifying function at the time of melting glass raw materials is decreased. Accordingly, it is preferably 0.005% by mass or greater and more preferably 0.01% by mass or greater. When the content of Cl exceeds 0.35% by mass, moisture concentration in glass is decreased and thus the clarity is degraded. Accordingly, it is preferably 0.25% by mass or less and more preferably 0.2% by mass or less.
Further, it is preferable that the total content of the halogen elements is 0.001% by mass or greater. When the content is less than 0.001% by mass, the clarifying function at the time of melting glass raw materials is decreased. Accordingly, it is preferably 0.01% by mass or greater and more preferably 0.03% by mass or greater.
In addition, it is preferable that the total content of the halogen elements is 1% by mass or less. When the content exceeds 1% by mass, strain point may be extremely decreased. Accordingly, it is preferably 0.7% by mass or less and more preferably 0.5% by mass or less.
Further, in order not to degrade characteristics of a metal or oxide thin film to be provided on the glass surface at the time of producing a panel, the alkali-free glass substrate of the present invention does not contain an alkali metal oxide more than an impurity level (substantially not). Moreover, in order to facilitate recycling of the glass, it is preferable that PbO, As2O3, and Sb2O3 are substantially not contained.
Further, for the same reason described above, it is preferable that P2O5 is substantially not contained. The amount to be mixed as an impurity is preferably 23 ppm by mole or less, more preferably 23 ppm by mole or less, still more preferably 18 ppm by mole or less, and particularly preferably 11 ppm by mole or less.
In order to improve meltability, clarity and formability at the time of producing glass, the total amount of 5% or less of ZnO and SO3 can be added to the alkali-free glass substrate of the present invention in addition to the components described above.
The alkali-free glass of the present invention has a strain point of preferably 680° C. or higher, more preferably 690° C. or higher, still more preferably 700° C. or higher, and still more preferably 710° C. or higher.
The alkali-free glass of the present invention has a Young's modulus of preferably 78 GPa or greater, or 79 GPa or greater, or 80 GPa or greater, still more preferably 81 GPa or greater, and still more preferably 82 GPa or greater.
The alkali-free glass substrate of the present invention has a UV transmittance at a wavelength of 300 nm of 40% to 85% in terms of 0.5 mm thickness.
At the time of producing an FPD, UV rays to be used for bonding two sheets of substrate glass constituting the FPD to each other, are mainly UV rays having a wavelength around a wavelength of 300 nm. When two sheets of substrate glass have small UV transmittance at a wavelength of 300 nm, it takes a long time for two sheets of substrate glass to be bonded to each other by using a UV curable resin. In other words, even when the UV curable resin is irradiated with UV rays, the rays are easily absorbed by the substrate glass and thus it takes a long time for the resin to be cured.
Since the alkali-free glass substrate of the present invention has a UV transmittance at a wavelength of 300 nm of 40% or greater in terms of 0.5 mm thickness, it does not take a long time for a UV curable resin to be cured when it is used as substrate glass constituting an FPD.
The UV transmittance of glass substrate varies depending on the thickness of the substrate. In the present invention, in order to exclude the influence due to the thickness of the substrate, it is standardized as a UV transmittance in terms of 0.5 mm thickness.
The UV transmittance at a wavelength of 300 nm is preferably 45% or greater and more preferably 50% or greater.
In this case, when the UV transmittance is excessively high, at the time of application of UV rays, characteristics of a TFT element are changed, for example, a Vth characteristic shift in the oxide semiconductor occurs, and the characteristics of constituent elements of an FPD may be degraded.
Since the alkali-free glass substrate of the present invention has a UV transmittance at a wavelength of 300 nm of 85% or less in terms of 0.5 mm thickness, there is no concern that the constituent elements of an FPD with a problem of heat resistance are damaged at the time of application of UV rays. It is preferably 80% or less and more preferably 75% or less.
In addition to an UV transmittance at a wavelength of 300 nm being within the above-described range, the alkali-free glass substrate of the present invention has a small in-plane distribution of the UV transmittance. Specifically, the in-plane distribution of UV transmittance at a wavelength of 300 nm is 1% or less and preferably 0.5% or less in a G6-sized substrate (typically, 1850 mm×1500 mm) in terms of 0.5 mm thickness. Therefore, in a case of being used as a substrate glass constituting an FPD, the application conditions of UV rays do not need to be changed according to the region of the substrate glass.
The alkali-free glass substrate of the present invention has an in-plane distribution of UV transmittance at a wavelength of 300 nm of preferably 1% or less and more preferably 0.5% or less in a G7-sized substrate (typically, 1870 mm×2200 mm) in terms of 0.5 mm thickness, and more preferably 1% or less and more preferably 0.5% or less in a G8-sized substrate (typically, 2460 mm×2160 mm) in terms of 0.5 mm thickness.
In the present specification, not limited to the transmittance, the “in-plane distribution” indicates a difference between the maximum value and the minimum value among the values in the plane.
In the alkali-free glass substrate of the present invention, in order that the UV transmittance and the in-plane distribution thereof satisfy the above-described numerical ranges, the average cooling rate and the in-plane distribution thereof around the glass transition point obtained by a rate cooling method satisfy the conditions described below.
As a result of intensive research on the in-plane distribution of UV transmittance in an alkali-free glass substrate by the present inventors, the following findings were obtained.
(1) In the case where an alkali-free glass substrate contains Fe, UV transmittance thereof is changed depending on the ratio of divalent iron to the total iron (so-called Redox) contained in the alkali-free glass substrate. Accordingly, when in-plane distribution of Redox is present in the alkali-free glass substrate, in-plane distribution of the UV transmittance is generated.
Further, even when in-plane distribution is present in the content of Fe in the alkali-free glass substrate, the in-plane distribution of the UV transmittance may be generated. For this reason, it is preferable that the in-plane distribution of the content of Fe is also small. In this case, however, minimizing the in-plane distribution of the concentration of Fe to an extreme level accompanies difficulty in production. In the present invention, the in-plane distribution of the content of Fe (in terms of Fe2O3) is preferably from 0.001% to 0.003%. In order to achieve the in-plane distribution of the content of Fe (in terms of Fe2O3) being less than 0.001%, it is necessary to more decrease the cooling rate than in the condition described below or to greatly increase the heater density, which accompanies difficulty in production. Meanwhile, when it exceeds 0.003%, the in-plane distribution of the UV transmittance may be generated.
(2) Redox of an alkali-free glass substrate is changed depending on melting temperature or cooling rate at the time of producing glass and the in-plane distribution of Redox of the alkali-free glass substrate is mainly affected by the cooling rate at the time of producing glass.
(3) The cooling rate of glass is not uniform and depending on the process of producing glass, and the cooling rate varies depending on the temperature range. However, since a linear relationship is established between fictive temperature of glass obtained by being cooled (rate cooling) from a high temperature at a constant cooling rate and the cooling rate, the fictive temperature can be alternatively defined as a cooling rate at the time of rate cooling. In the present specification, this is set as an average cooling rate around glass transition point obtained by a rate cooling method. The average cooling rate around glass transition point obtained by a rate cooling method can be obtained by following the procedures described below in detail.
A test of cooling glass at a constant cooling rate is performed at 0.1° C./min, 1° C./min, 10° C./min, 100° C./min, and 1000° C./min after holding the glass at a temperature which is approximately 100° C. higher than the glass transition point for 10 minutes. The relationship between refractive index and the cooling rate can be obtained as a calibration curve by measuring the refractive indices of all sheets of glass. Subsequently, the refractive index of an actual sample is measured and the cooling rate thereof is obtained from the calibration curve.
Hereinafter, in the present specification, when the “average cooling rate” is noted, this term indicates the average cooling rate around glass transition point obtained by using the rate cooling method.
(4) When the average cooling rate is set to a predetermined numerical value or less and the in-plane distribution thereof is decreased, the in-plane distribution of Redox of an alkali-free glass substrate can be decreased and the in-plane distribution of UV transmittance can be decreased.
The alkali-free glass substrate of the present invention has the average cooling rate of 400° C./min or less and the in-plane distribution of the average cooling rate of 40° C./min or less.
When the average cooling rate of an alkali-free glass substrate is 400° C./min or less, UV transmittance of the alkali-free glass substrate falls within the above-described range and the in-plane distribution of the UV transmittance becomes smaller.
When the in-plane distribution of the average cooling rate of an alkali-free glass substrate is 40° C./min or less (±20° C./min or less), the in-plane distribution of UV transmittance of the alkali-free glass substrate becomes sufficiently small, and becomes 1% or less in a G6-sized substrate in terms of 0.5 mm thickness.
In the alkali-free glass substrate of the present invention, it is preferable that the average cooling rate is 300° C./min or less and the in-plane distribution of the average cooling rate is 40° C./min or less (±20° C./min or less), more preferable that the average cooling rate is 220° C./min or less and the in-plane distribution of the average cooling rate is 30° C./min or less (±15° C./min or less), and particularly preferable that the average cooling rate is 150° C./min or less and the in-plane distribution of the average cooling rate is 30° C./min or less (±15° C./min or less).
For example, the alkali-free glass substrate of the present invention can be produced according to the following method. Raw materials of respective components being normally used are prepared so as to have target components such that strain point is 680° C. or higher, Young's modulus is 78 GPa or greater, and UV transmittance at a wavelength of 300 nm is from 40% to 85% in terms of 0.5 mm thickness, continuously put this into a melting furnace, and heated in a temperature of from 1500° C. to 1800° C. to be melted. The molten glass is formed to have a predetermined thickness by using various forming methods (a float method, a down draw method, a fusion method, etc.) and cut after being annealed, thereby obtaining an alkali-free glass substrate.
In the present invention, the temperature conditions at the time of forming and annealing need to be managed such that the average cooling rate becomes 400° C./min or less, the in-plane distribution of the average cooling rate becomes 40° C./min or less, and the in-plane distribution of UV transmittance at a wavelength of 300 nm in a G6-sized substrate becomes 1% or less in terms of 0.5 mm thickness. Here, in order to decrease the in-plane distribution of the average cooling rate, it is preferable to heat a glass ribbon from the side surface side at the time of forming and annealing.
Hereinafter, examples 1, 3, 5, 7, 9, 11, 13, 15, 17, 19, 21, 23, 25, 27, 29, 31, 33, 35, 37, 39, 41, 43, 45, and 47 are Examples and examples 2, 4, 6, 8, 10, 12, 14, 16, 18, 20, 22, 24, 26, 28, 30, 32, 34, 36, 38, 40, 42, 44, 46, and 48 are Comparative Examples.
Raw materials of respective components are prepared to have a target composition and melted. In Examples, the heat retention in side wall portions of a forming furnace and an annealing furnace is strengthened, the temperature distribution of a heater in the annealing furnace is adjusted by focusing on the temperature distribution of glass, and the temperature distribution of the glass is made to be better (uniform) than that in the conventional art. In Comparative Examples, the heat retention of side wall portions of the forming furnace and the annealing furnace is as usual and the heat retention thereof is weak compared to that of Examples, and the temperature distribution of the heater in the annealing furnace is adjusted in the manner of the conventional art without focusing on the minute temperature distribution of glass.
Table 1 shows the glass compositions (unit: % by mass) of glasses 1 to 8, the thermal expansion coefficient (unit: ×10−7/° C.) at a temperature of from 50° C. to 350° C., the strain point (unit: ° C.), the glass transition point (unit: ° C.), the specific gravity, the Young's modulus (GPa) (measured by an ultrasonic method), a temperature T2 as an index of meltability (temperature at which glass viscosity η becomes 102 poise, unit: ° C.) and a temperature T4 as an index of float formability and fusion formability (temperature at which the glass viscosity η becomes 104 poise, unit: ° C.) as values of high temperature viscosity, the devitrification temperature (unit: ° C.), and the photoelastic constant (unit: nm/MPa/cm) (measured by using a disk compression method at a measurement wavelength of 546 nm). Table 2 shows glasses used in Examples 1 to 48, the average cooling rate (unit: ° C./min), the in-plane distribution of the average cooling rate (unit: ° C./min), the average in-plane transmittance (unit: %) at a wavelength of 300 nm, and the in-plane distribution of the transmittance (unit: %) at a wavelength of 300 nm. In addition, the size of the glass used in each of Examples is the G6 size (1850 mm×1500 mm×0.5 mm).
The average in-plane transmittance and the in-plane distribution of the transmittance can be obtained by cutting a G6-sized plate into a plurality of samples of 50 mm×50 mm and measuring the transmittance and the refractive index of each sample. The transmittance of glass was measured by using a Hitachi ultraviolet-visible near-infrared spectrophotometer 4U-4100. The refractive index was measured by using a precision refractometer KPR-2000 manufactured by Shimadzu Device Corporation.
TABLE 1
% by mass
Glass 1
Glass 2
Glass 3
Glass 4
Glass 5
Glass 6
Glass 7
Glass 8
SiO2
60.9
60.9
61.3
61.3
60.5
59.3
61.6
63.6
Al2O3
19.7
19.7
20.4
20.5
18.8
20.0
19.7
20
B2O3
2.5
2.5
1
1
4.8
1.8
3.7
0
MgO
5.2
5.2
5.7
5.7
4.3
4.1
3.8
7
CaO
4.4
4.4
4.5
4.5
4.1
1.6
5.5
9.4
SrO
7
7
6.9
6.9
7.5
8.7
5.7
0
BaO
0
0
0
0
0
4.5
0
0
SnO2
0.20
0.18
0.15
0.10
0.10
0.05
0.03
0.50
F
0.07
0.07
0
0
0
0.07
0.07
0
Cl
0.2
0
0
0.06
0.06
0.2
0.2
0
Fe2O3
0.04
0.015
0.04
0.015
0.008
0.027
0.05
0.017
Average thermal
39
39
39
39
39
40
39
40
expansion coefficient
[×10−7/° C.]
Strain point [° C.]
710
710
723
723
693
712
715
733
Glass transition
775
775
790
790
750
793
762
792
point [° C.]
Specific gravity
2.57
2.57
2.59
2.59
2.55
2.61
2.53
2.55
Young's modulus
84
84
87
87
82
82
82
91
[GPa]
T2 [° C.]
1650
1650
1650
1650
1640
1702
1660
1622
T4 [° C.]
1290
1290
1295
1295
1287
1333
1300
1281
Devitrification
1280
1280
1290
1290
1235
1312
1265
1255
temperature [° C.]
Photoelastic constant
28
28
27
27
28
27
28
26
[nm/MPa/cm]
TABLE 2
Average
Average cooling
Average in-plane
Transmittance
Used
cooling rate
rate distribution
transmittance
distribution
Examples
glass
[° C./min]
[° C./min]
at 300 nm [%]
at 300 nm [%]
Example 1
Glass 1
350
30
41.9
0.3
Example 2
350
120
41.9
1.1
Example 3
150
20
48.5
0.9
Example 4
150
50
48.5
2.2
Example 5
40
5
56.6
0.8
Example 6
40
50
56.6
4.8
Example 7
Glass 2
350
30
71.3
0.3
Example 8
350
100
71.3
1.1
Example 9
150
30
73.9
0.9
Example 10
150
50
73.9
2.2
Example 11
40
8
76.7
0.8
Example 12
40
50
76.7
4.8
Example 13
Glass 3
350
30
46.9
0.3
Example 14
350
100
46.9
1.1
Example 15
150
30
52.8
0.9
Example 16
150
50
52.8
2.2
Example 17
40
8
58.5
0.8
Example 18
40
50
58.5
4.8
Example 19
Glass 4
350
30
72.2
0.3
Example 20
350
100
72.2
1.1
Example 21
150
30
74.8
0.9
Example 22
150
50
74.8
2.2
Example 23
40
8
77.2
0.8
Example 24
40
50
77.2
4.8
Example 25
Glass 5
350
30
80.1
0.3
Example 26
350
100
80.1
1.1
Example 27
150
30
81.4
0.9
Example 28
150
50
81.4
2.2
Example 29
40
8
82.7
0.8
Example 30
40
50
82.7
4.8
Example 31
Glass 6
350
30
58.3
0.3
Example 32
350
100
58.3
1.1
Example 33
150
30
61.6
0.9
Example 34
150
50
61.6
2.2
Example 35
40
8
65.1
0.8
Example 36
40
50
65.1
4.8
Example 37
Glass 7
350
30
40.4
0.3
Example 38
350
100
40.4
1.1
Example 39
150
30
43.4
0.9
Example 40
150
50
43.4
2.2
Example 41
40
8
46.6
0.8
Example 42
40
50
46.6
4.8
Example 43
Glass 8
350
30
69.0
0.3
Example 44
350
100
69.0
1.1
Example 45
150
30
71.4
0.9
Example 46
150
50
71.4
2.2
Example 47
40
8
73.9
0.8
Example 48
40
50
73.9
4.8
As is obvious from Tables, in all sheets of glass in Examples, since the in-plane distribution of the average cooling rate is 40° C./min or less and the in-plane distribution of the UV transmittance at a wavelength of 300 nm in a G6-sized substrate is 1% or less, it is considered that the yield thereof is improved when used as an FPD substrate glass.
The present invention has been described in detail with reference to specific embodiments thereof, but it will be apparent to a person skilled in the art that various changes and modifications can be made without departing from the spirit and scope of the present invention.
The present application is based on Japanese Patent Application No. 2013-090141 filed on Apr. 23, 2013, the contents of which are incorporated herein by reference.
Since the alkali-free glass substrate of the present invention is easily formed to have a plate shape and the in-plane distribution of UV transmittance is suppressed, it is suitable for a substrate glass for various kinds of displays.
Kunigita, Masaya, Koike, Akio, Tokunaga, Hirofumi
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